Next, we study the behavior in the absence of external magnetic field but in presence of strain induced gauge field \(B_5\) . First, similar to the case with TR broken Weyl semimetals, we find that strain induced chiral magnetic field \(B_5\)  always results in a negative LMC coefficient \(\sigma _{zz}^{(2)}\) . This results in in contradiction to earlier claims that find an increase in longitudinal magnetoconductivity with strain [1]}, [2]}. The reason can be traced out to the non-inclusion of intervalley scattering, momentum dependent scattering, and charge conservation, all of which are included in the current work (see Appendix A).
Furthermore, we find that strain, by itself results in strong sign-reversal, while tilting results in weak sign reversal.
In Fig. REF  (a) we plot LMC as a function of strain induced magnetic field \(B_5\) , which clearly demonstrates these features.
As before, we fit the magnetoconductivity via the following expression
\(\sigma _{zz}(B_5)= \sigma _{zz}^{(2)}(B-B_{50})^2 + \sigma _{zz}(B_{50}),\) 
